A GENERIC TECHNIQUE FOR ACOUSTIC EMISSION SOURCE LOCATION
|
|
- Barnard Nigel Ward
- 5 years ago
- Views:
Transcription
1 A GENERIC TECHNIQUE FOR ACOUSTIC EMISSION SOURCE LOCATION JONATHAN J. SCHOLEY 1,2, PAUL D. WILCOX 2, MICHAEL R. WISNOM 1, MIKE I. FRISWELL 1, MARTYN PAVIER 2 and MOHAMMAD R ALIHA 3 1) Department of Aerospace Engineering, University of Bristol, Bristol, BS8 1TR, UK; 2) Department of Mechanical Engineering, University of Bristol, Bristol, BS8 1TR, UK; 3) Fatigue and Fracture Laboratory, Department of Mechanical Engineering, Iran University of Science and Technology, Narmak, 16846, Tehran, Iran Abstract Acoustic emission (AE) source location is an essential part of any quantitative AE test as it provides information about damage mechanisms and allows spatial separation so that signals from unwanted sources can be eliminated. In this paper, an AE source location technique described as the best-matched point search method is presented. The application of the bestmatched point search method is demonstrated in two source location experiments: one on a large anisotropic carbon-fibre composite (CFC) plate and one on a thick oolitic limestone disc. In the large composite plate test, source location is achieved using the S 0 mode, which displays a complicated group velocity pattern. In the oolitic limestone experiment, three-dimensional source location is demonstrated. The best-matched point search method successfully determines the location of AE sources in both tests. Errors in source location are attributed to the extraction of delta-t times from the AE signals. Keywords: Source location, Best-matched point search method, Carbon-fibre composite, Limestone Introduction Acoustic emission (AE) source location is an essential part of any quantitative AE test. In addition to confirming the spatial origin of AE signals, AE source location can be used to selectively eliminate AE signals from unwanted acoustic sources and provide useful information about the development of damage mechanisms [1]. Further, in quantitative source characterisation experiments, AE source location is used to determine the distance between the acoustic source and AE sensors, which is subsequently used to remove propagation effects from measured signals [1-4]. The majority of reported AE source location techniques involve two independent stages which can be considered separately: the measurement of arrival times from received waveforms and the use of these arrival times to determine the origin of the acoustic source. The work in this paper is concerned with the latter of these two stages. An AE source location technique described as the best-matched point search method is presented. The best-matched point search method is an approach, which builds on ideas mentioned by Tobias [5]. The technique was first introduced in a recent conference paper [3] and is expanded upon in this paper to demonstrate its application to three-dimensional solids. The technique was originally developed to determine the origin of acoustic events in plates with complex angular group-velocity patterns and an example of its application to a cross-ply carbon-fibre composite (CFC) plate is given. AE source location for plates with circular or elliptical group J. Acoustic Emission, 27 (2009) Acoustic Emission Group
2 velocity patterns, found in composite plates with quasi-isotropic or uni-directional lay-ups respectively, can be determined analytically using algorithms proposed by Tobias [5], Paget et al. [6] and Kurokawa et al. [7]. Some composite plates, frequently used in laboratory-based source characterisation experiments, contain lay-ups, which lead to complicated angular group-velocity patterns [8, 9]. Analytical two-dimensional source location in plates with complicated groupvelocity patterns is exceptionally challenging and as a result, a generic technique for determining the location of acoustic sources on plates with any angular group-velocity pattern is highly desirable. Although some success in this area has already been achieved using iterative convergence schemes [4, 10, 11], the authors are unaware of any literature, which describes source location using group-velocity patterns as complicated as the S 0 mode in cross-ply composite plates. The best-match point search method is a generic source-location technique and as a second example, the technique is used to determine the three-dimensional source location of Hsu- Nielsen pencil-lead breaks (PLBs) in an oolitic limestone disc. The results of the AE source location testing on the oolitic limestone disc demonstrate the versatility of the technique. The practical application of the best-matched point search method and suggestions for how the technique can be applied in specimens with more complicated geometries are discussed. The Best-Matched Point Search Method The best-matched point search method is a simple numerical approach for determining AE source location. The method is broken down into two stages: point generation and point matching. In the point generation stage, the specimen geometry is represented by an array of points with spatial location vectors r. The theoretical time, t i, taken for an elastic wave to propagate from a point, r, to the i th sensor is given by: where s i is the spatial location vector of the i th sensor and v gr is the group velocity of the elastic wave, which is a function of the propagation direction between the sensor and point. The unit vector, e, which describes the propagation direction between the i th sensor and a point is given by: The difference in arrival time between two sensors (known as a delta-t time, Δt) is then calculated for each point in the array. With the exception of certain ambiguous points, discussed later in this section, each point has a unique combination of delta-t values, which corresponds to a location on the plate. The array of delta-t values only needs to be compiled once for any given specimen/sensor configuration: (1) (2) where i and j denote sensor locations. (3) In the point matching stage, the delta-t array is searched for the best match to the experimentally measured delta-t values. The estimated position of the source, r, is given by: (4) 292
3 where t exp are the experimentally measured delta-t values. The summation is applied for every independent combination of delta-t values, N, which for a number of sensors, S, is given by: (5) It should be noted that certain combinations of delta-t times are ambiguous and in these situations, a source location is not unique [3, 5]. If two points on the specimen are separated by a large distance and have similar delta-t values, then an error in the source location can occur. Unique combinations of delta-t values can be obtained by adding sensors to the specimen and increasing the number of independent delta-t values. The topic of ambiguous delta-t values is described by Tobias [5] with visual examples of the problem presented by Scholey et al. [3]. Application of the Best-Matched Point Search Method to Two-Dimensional Plates To demonstrate the source location capability of the best-matched point search method on anisotropic plates, a source location test was conducted on a large, cross-ply CFC plate. The plate was constructed from uni-directional SE84HT prepreg with a lay-up [(0, 90) 6 ] s. The plate was 3.6-mm thick and had in-plane dimensions of 1166 x 924 mm. Experimental measurements of the S 0 group velocity were made on the plate. The measurements were made in different directions relative to the surface ply, between 0 o and 90 o at 10 o intervals. A 2-cycle Hanningwindowed toneburst with a centre frequency of 150 khz was used to pulse a transducer at the centre of the plate. A second transducer, located 294 mm away, was placed at different angular locations and the arrival time of the S 0 signal used to calculate the group velocity in that direction. The delay in the equipment was measured and accounted for in the group velocity calculation. Figure 1 shows the experimental points measured. It should be noted that measurements were only taken between 0 o and 90 o and that the points between 90 o and 360 o are only shown for completeness. It can be seen that the angular group-velocity pattern of the S 0 mode is neither circular nor elliptical and therefore source location on this plate cannot be solved analytically using the methods reported in the literature [5-7]. Fig. 1: S 0 -mode group velocity in different directions on a SE84HT [(0, 90) 6 ] s plate. 293
4 Three AE sensors were mounted on the plate at locations (450, 350), (750, 350) and (450, 650) with units in mm. The AE sensors were manufactured from cylindrical pz-27 piezoelectric elements, with a diameter of 3 mm and a height of 3 mm. The sensors were attached to the plate using commercial superglue. A 0.5-mm Hsu-Nielsen pencil-lead break (PLB) was used as an acoustic source at 13 different locations on the plate. Due to the high attenuation of ultrasonic waves in the CFC plate at 150 khz and the low excitability of the S 0 mode, the locations of the PLB sources were chosen to ensure that each sensor could measure the S 0 -mode signals. The received signals were amplified using Physical Acoustic Corporation (PAC) 2/4/6 amplifiers and were received on a LeCroy 6030 Waverunner digital oscilloscope. To obtain delta-t values, the signals were frequency-filtered with a raised cosine window centred on 150 khz and a bandwidth of 300 khz. The filtered signals were enveloped and the arrival time determined using a threshold amplitude just above the noise level. Delta-t values were calculated using Eq. (3). Figure 2(a) shows the estimated source location for the 13 different points, calculated using the mean group velocity of 5.35 mm µs -1 (i.e., the average at all angles). With the exception of the points near the centre of the sensor array, where the propagation directions of all ray-paths from the source to the sensors is similar, the source location is quite poor. Figure 2(b) shows the estimated source location using the measured group-velocity pattern with a point array resolution of 2 mm. It can be seen that the estimated source locations are in good agreement with the actual source locations. Only one point, far from the centre of the sensor array provides any substantial error. It should be noted that the errors in the extraction of the arrival times from measured waveforms are automatically incorporated in these plots. (a) Fig. 2: Source location on the SEHT84 CP CFC plate. (a) average group velocity, (b) S 0 group velocity profile (Sensor locations o, true PLB locations, estimated PLB locations x ). Application of the Best-Matched Point Search Method to Three-Dimensional Solids The best-matched point search method is a generic source location technique, which can be applied to different types of structure. The ability of the technique to locate acoustic sources in plates with complex group-velocity patterns was demonstrated in the previous section. In this section, the technique is used to determine the source location of PLBs in a thick oolitic lime- (b) 294
5 stone disc. Oolitic limestone is a soft, homogenous rock, which is a composed of calcite. The rock, widely found in the UK, is porous and beige in color. Elastic wave propagation in the limestone disc at ultrasonic frequencies is assumed to be dominated by bulk waves. The oolitic limestone disc is assumed to be isotropic and as a result, the propagation velocity is equal in all directions. The velocity of a longitudinal wave propagating through the oolitic limestone was determined experimentally using ASTM standard D [12]. A cylindrical oolitic limestone specimen, diameter 47 mm and length 100 mm, was used in the velocity test. A 2-cycle Hanning-windowed tone-burst with a centre frequency of 250 khz, generated by an Agilent 33220A Arbitrary Waveform Generator, was used to pulse a piezoelectric transducer. The transducer was manufactured from a PCM51 cylindrical element with a diameter of 3 mm and a height of 3 mm. The transducer was mounted at the centre of the face on one end of the specimen. At the opposite end of the specimen, a second PCM51 transducer was used to receive the elastic wave energy. The received signal was amplified using a PAC 2/4/6 amplifier and recorded using a LeCroy 6030 Waverunner digital oscilloscope, which also captured the output signal from the waveform generator. Due to the high attenuation of elastic wave energy in the oolitic limestone material at 250 khz, the signal-to-noise ratio was improved by averaging the received signal 10,000 times. The time taken for the wave to propagate along the length of the specimen was taken to be the difference in arrival times of the output signal from the waveform generator and the arrival of the signal from the propagated wave. A system delay of 1.1 µs was determined and accounted for in the calculation. The group velocity was estimated as 3.34 mm µs -1. ASTM Standard D [12] presents a crude method for measuring the velocity of elastic waves since material attenuation and energy spreading lead to changes in the waveform shape and amplitude. In the absence of a phase delay technique [13], an improvement in the propagation time estimation time was sought by enveloping the signals used in the calculation. The application of the signal envelopes gave a new propagation time and an estimated group velocity of 3.06 mm µs -1. The measured velocity is in the range reported for limestone material [14]. The source location test was conducted on an oolitic limestone disc. The disc was 30-mm thick and had a diameter of 100 mm. A flat slit, width 30 mm, passed through the entire thickness of the disc. The purpose of the slit was to act as a crack initiator in an unrelated series of tests. Four AE sensors were mounted on the side of the disc on the mid-plane at regular intervals. The AE sensors were manufactured from cylindrical pz-27 piezoelectric elements, with a diameter of 3 mm and a height of 3 mm. The sensors were attached to the plate using commercial superglue. A 0.3-mm Hsu-Nielsen pencil-lead break (PLB) was used as an acoustic source at 17 different locations on the upper surface of the disc. The signals were amplified using PAC 2/4/6 amplifiers set at 40 db gain and were captured on a PAC PCI-2 AE system. The arrival times of the signals were obtained by using a threshold crossing technique applied to the enveloped raw signals. The threshold amplitude was set a few db about the ambient noise level. Delta-t values were then calculated using Eq. (2). A three-dimensional array of points with a resolution of 1 mm was established and was searched in the best-matched point search method. Since the experiment is symmetrical about the mid-plane of the disc, only one half of the disc is considered in the point array. Figure 3 shows the estimated source location for the 17 different points, calculated using a bulk wave velocity of 3.06 mmµs -1. At each PLB location (marked ), the estimated throughthickness location of the source is also given; the range is from 0 mm (the mid-plane of the disc) 295
6 up to 15 mm (the upper surface where the PLBs were applied). It can be seen that for all events, the lateral location of the PLB source as estimated by the best-point search method is good. In most cases, the best-point search technique also successfully identifies the through-thickness location of the source. However, there are large errors in the estimated through-thickness location of the PLB source at five locations, with errors in through-thickness location of up to 15 mm. Fig. 3: Source location results for the oolitic limestone disc experiment (Sensor locations o, true PLB locations, estimated PLB locations x, numeric subscripts describe estimated through-thickness location). Discussion The best-matched point search technique relies on delta-t values obtained from experimental AE signals. In this work, arrival times were measured from enveloped RF signals using a threshold crossing technique. Threshold crossing techniques are frequently used in AE testing to determine the arrival of signals, but errors can exist in the measured arrival times, which lead to errors in delta-t times and estimated location. A second source of error is the elastic wave velocity used to calculate the theoretical propagation times in the point array. In the absence of known material properties, the elastic wave velocity must be determined experimentally. In this work, the elastic wave velocity was determined experimentally for both specimens. The sensitivity of the reported source location with respect to changes in delta-t value can vary and is dependent both on the position of the acoustic source and the configuration of the sensors [3]. In regions outside the sensor array, the location resolution decreases rapidly and as a result, a small change in a delta-t value leads to a large change in the estimated source location. The reduction in source location resolution exaggerates any errors in the assumed velocity and/or experimental delta-t values. The effects of poor location resolution are seen in both tests. In the 296
7 CFC plate test, larger errors occur away from the centre of the sensor array. In the limestone disc location test, all of the sensors were mounted on the mid-plane of the specimen and as a result, the specimen had a poor location resolution in the through-thickness direction. Consequently, the source location in the plane parallel to the mid-plane of the disc was excellent but the estimated through-thickness location of some events was poor. The best-matched point search method is a simple, generic technique, which can be applied to many practical structures. The technique relies on the generation of a point array, which for some geometries could be difficult to generate. In this work, the point arrays used for both tests were generated in Matlab and had a regular spacing in all spatial dimensions. An example of a regularly spaced point array is shown in Fig. 4(a). More sophisticated arrays can be used. For example, Fig. 4(b) shows an array where the spacing of the points varies on the specimen. Such an array could be used in a test where the acoustic source is expected to occur in the centre of the specimen, allowing improved resolution where desired without increasing the total number of points that need to be searched. Further, the powerful meshing algorithms in finite element software could be used to generate the co-ordinates for the point arrays in more complex geometries" (a) Regular spacing. Fig. 4: Point arrays. (b) Variable spacing. Conclusions The best-matched point search method has been used to determine the source location of PLBs on an anisotropic cross-ply CFC plate and in a thick oolitic limestone disc. Source location on the anisotropic plate was determined using the S 0 -mode signals, which have a complicated group-velocity pattern. Source location on the oolitic limestone disc gave both in-plane and through-thickness source location. Errors in both tests have been attributed to errors in the capture of delta-t times from the AE signals, errors in the assumed elastic wave velocity and the position of the source relative to the sensors. The applicability of non-regular point arrays has been discussed and it has been noted that the approach may be extended to more complicated geometries using the powerful meshing algorithms in finite element software. 297
8 Acknowledgements This work was supported by the UK Engineering and Physical Sciences Research Council (EPSRC) through the UK Research Centre in NDE (RCNDE) and by Airbus, Rolls-Royce and Nexia Solutions. The authors are grateful to Mike Lowe of Imperial College for the loan of the large cross-ply CFC plate. References [1] Scholey J.J.: PhD Thesis, University of Bristol, UK, [2] Scholey J.J., Wilcox P.D., Lee C.K., Friswell M.I., Wisnom M.R.: Proceedings of the 27 th European Conference on Acoustic Emission Testing, September 2006, Cardiff, UK, pp [3] Scholey J.J., Wilcox P.D., Lee C.K., Friswell M.I., Wisnom M.R.: Proceedings of the 28 th European Conference on Acoustic Emission Testing, September 2008, Cracow, Poland, pp [4] Kinjo T., Suzuki H., Takemoto M., Ono K.: Japanese Journal of Applied Physics, 36, 1997, [5] Tobias A.: Non-Destructive Testing, 9, 1976, [6] Paget C.A., Atherton K., O Brien E.: Proceedings of the 4 th International Workshop on Structural Health Monitoring, 2003, Stanford, CA, pp [7] Kurokawa Y., Mitzutani Y., Mayuzumi M.: Journal of Acoustic Emission, 23, 2005, [8] Neau G., Lowe M.J.S., Deschamps M.: Quantitative Non-Destructive Evaluation, 21, 2002, [9] Neau G.: PhD Thesis, Imperial College London, UK, [10] Toyama N., Koo J.H., Oishi R.: Journal of Materials Science Letters, 20, 2001, [11] Yamada H., Mizutani Y., Nishino H., Takemoto M., Ono K.: Journal of Acoustic Emission, 18, 2000, [12] ASTM Standard D Standard Test Method for Laboratory Determination of Pulse Velocities and Ultrasonic Constants of Rock, [13] Sachse W., Pao Y.H.: Journal of Applied Physics, 49 (8), 1978, [14] Hardy H. R.: Acoustic Emission/Microseismic Activity: Volume 1: Principles, Techniques and Geotechnical Applications, Balkema Publisher, Netherland,
DAMAGE IN CARBON FIBRE COMPOSITES: THE DISCRIMINATION OF ACOUSTIC EMISSION SIGNALS USING FREQUENCY
DAMAGE IN CARBON FIBRE COMPOSITES: THE DISCRIMINATION OF ACOUSTIC EMISSION SIGNALS USING FREQUENCY MARK EATON, KAREN HOLFORD, CAROL FEATHERSTON and RHYS PULLIN Cardiff School of Engineering, Cardiff University,
More informationQuantitative structural health monitoring using acoustic emission
Quantitative structural health monitoring using acoustic emission Paul D. Wilcox *1, Chee Kin Lee 1, Jonathan J. Scholey 2, Michael I. Friswell 2, Michael R. Wisnom 2 and Bruce W. Drinkwater 1 1 Department
More informationEWGAE 2010 Vienna, 8th to 10th September
EWGAE 2010 Vienna, 8th to 10th September Frequencies and Amplitudes of AE Signals in a Plate as a Function of Source Rise Time M. A. HAMSTAD University of Denver, Department of Mechanical and Materials
More informationNOVEL ACOUSTIC EMISSION SOURCE LOCATION
NOVEL ACOUSTIC EMISSION SOURCE LOCATION RHYS PULLIN, MATTHEW BAXTER, MARK EATON, KAREN HOLFORD and SAM EVANS Cardiff School of Engineering, The Parade, Newport Road, Cardiff, CF24 3AA, UK Abstract Source
More informationTime Reversal FEM Modelling in Thin Aluminium Plates for Defects Detection
ECNDT - Poster 39 Time Reversal FEM Modelling in Thin Aluminium Plates for Defects Detection Yago GÓMEZ-ULLATE, Instituto de Acústica CSIC, Madrid, Spain Francisco MONTERO DE ESPINOSA, Instituto de Acústica
More informationInstantaneous Baseline Damage Detection using a Low Power Guided Waves System
Instantaneous Baseline Damage Detection using a Low Power Guided Waves System can produce significant changes in the measured responses, masking potential signal changes due to structure defects [2]. To
More informationTHE EXTRACTION METHOD FOR DISPERSION CURVES FROM SPECTROGRAMS USING HOUGH TRANSFORM
THE EXTRACTION METHOD FOR DISPERSION CURVES FROM SPECTROGRAMS USING HOUGH TRANSFORM Abstract D.A. TERENTYEV, V.A. BARAT and K.A. BULYGIN Interunis Ltd., Build. 3-4, 24/7, Myasnitskaya str., Moscow 101000,
More informationCo-Located Triangulation for Damage Position
Co-Located Triangulation for Damage Position Identification from a Single SHM Node Seth S. Kessler, Ph.D. President, Metis Design Corporation Ajay Raghavan, Ph.D. Lead Algorithm Engineer, Metis Design
More informationPassive impact localisation for the structural health monitoring of new airframe materials
Journal of Physics: Conference Series OPEN ACCESS Passive impact localisation for the structural health monitoring of new airframe materials To cite this article: Jacob Ward et al 2013 J. Phys.: Conf.
More informationLocalization of Acoustic Emission Sources in Fiber Composites Using Artificial Neural Networks
31 st Conference of the European Working Group on Acoustic Emission (EWGAE) Fr.3.B.1 More Info at Open Access Database www.ndt.net/?id=17530 Localization of Acoustic Emission Sources in Fiber Composites
More informationEFFECTS OF LATERAL PLATE DIMENSIONS ON ACOUSTIC EMISSION SIGNALS FROM DIPOLE SOURCES. M. A. HAMSTAD*, A. O'GALLAGHER and J. GARY
EFFECTS OF LATERAL PLATE DIMENSIONS ON ACOUSTIC EMISSION SIGNALS FROM DIPOLE SOURCES ABSTRACT M. A. HAMSTAD*, A. O'GALLAGHER and J. GARY National Institute of Standards and Technology, Boulder, CO 835
More informationDETECTION AND SIZING OF SHORT FATIGUE CRACKS EMANATING FROM RIVET HOLES O. Kwon 1 and J.C. Kim 1 1 Inha University, Inchon, Korea
DETECTION AND SIZING OF SHORT FATIGUE CRACKS EMANATING FROM RIVET HOLES O. Kwon 1 and J.C. Kim 1 1 Inha University, Inchon, Korea Abstract: The initiation and growth of short fatigue cracks in a simulated
More informationRayleigh Wave Interaction and Mode Conversion in a Delamination
Rayleigh Wave Interaction and Mode Conversion in a Delamination Sunil Kishore Chakrapani a, Vinay Dayal, a and Jamie Dunt b a Department of Aerospace Engineering & Center for NDE, Iowa State University,
More informationULTRASONIC GUIDED WAVE ANNULAR ARRAY TRANSDUCERS FOR STRUCTURAL HEALTH MONITORING
ULTRASONIC GUIDED WAVE ANNULAR ARRAY TRANSDUCERS FOR STRUCTURAL HEALTH MONITORING H. Gao, M. J. Guers, J.L. Rose, G. (Xiaoliang) Zhao 2, and C. Kwan 2 Department of Engineering Science and Mechanics, The
More informationON LAMB MODES AS A FUNCTION OF ACOUSTIC EMISSION SOURCE RISE TIME #
ON LAMB MODES AS A FUNCTION OF ACOUSTIC EMISSION SOURCE RISE TIME # M. A. HAMSTAD National Institute of Standards and Technology, Materials Reliability Division (853), 325 Broadway, Boulder, CO 80305-3328
More informationThe Development of Laser Ultrasonic Visualization Equipment and its Application in Nondestructive Inspection
17th World Conference on Nondestructive Testing, 25-28 Oct 2008, Shanghai, China The Development of Laser Ultrasonic Visualization Equipment and its Application in Nondestructive Inspection Bo WANG 1,
More informationQuantitative Crack Depth Study in Homogeneous Plates Using Simulated Lamb Waves.
More Info at Open Access Database www.ndt.net/?id=18675 Quantitative Crack Depth Study in Homogeneous Plates Using Simulated Lamb Waves. Mohammad. (. SOORGEE, Aghil. YOUSEF)-KOMA Nondestructive Testing
More informationStructural Integrity Monitoring using Guided Ultrasonic Waves
Structural Integrity Monitoring using Guided Ultrasonic Waves Paul Fromme Department of Mechanical Engineering University College London NPL - May 2010 Structural Integrity Monitoring using Guided Ultrasonic
More informationPiezoelectric transducer excitation for guided waves propagation on pipeline with flexural wave modes
9 th European Workshop on Structural Health Monitoring July 10-13, 2018, Manchester, United Kingdom Piezoelectric transducer excitation for guided waves propagation on pipeline with flexural wave modes
More informationA Detailed Examination of Waveforms from Multiple Sensors on a Composite Pressure Vessel (COPV)
A Detailed Examination of Waveforms from Multiple Sensors on a Composite Pressure Vessel (COPV) By M. A. Hamstad University of Denver, Department of Mechanical and Materials Engineering Denver, CO USA
More informationMATERIALS CHARACTERIZATION USING LASER ULTRASONIC GUIDED WAVES
MATERIALS CHARACTERIZATION USING LASER ULTRASONIC GUIDED WAVES NDCM XII VA Tech June 19 to 24, 2011 B. Boro Djordjevic Materials and Sensors Technologies, Inc. Maryland, USA 410 766 5002, Fax. 410766 5009,
More informationEXPERIMENTAL TRANSFER FUNCTIONS OF PRACTICAL ACOUSTIC EMISSION SENSORS
EXPERIMENTAL TRANSFER FUNCTIONS OF PRACTICAL ACOUSTIC EMISSION SENSORS Kanji Ono 1 and Hideo Cho 2 1 University of California, Los Angeles, Los Angeles, CA 90095, USA 2 Aoyama Gakuin University, Sagamihara,
More informationCONTINUOUS DAMAGE MONITORING TECHNIQUES FOR LAMINATED COMPOSITE MATERIALS
CONTINUOUS DAMAGE MONITORING TECHNIQUES FOR LAMINATED COMPOSITE MATERIALS M. Surgeon, M. Wevers Department of Metallurgy and Materials Engineering (KULeuven), De Croylaan 2, B-31 Heverlee, Belgium SUMMARY:
More informationMeasurement of phase velocity dispersion curves and group velocities in a plate using leaky Lamb waves
Measurement of phase velocity dispersion curves and group velocities in a plate using leaky Lamb waves NDE2002 predict. assure. improve. National Seminar of ISNT Chennai, 5. 7. 12. 2002 www.nde2002.org
More informationUNDERSTANDING THE PROPAGATION OF GUIDED ULTRASONIC WAVES IN UNDAMAGED COMPOSITE PLATES
The 14 th International Conference of the Slovenian Society for Non-Destructive Testing»Application of Contemporary Non-Destructive Testing in Engineering«September 4-6, 2017, Bernardin, Slovenia More
More informationDAMAGE DETECTION IN PLATE STRUCTURES USING SPARSE ULTRASONIC TRANSDUCER ARRAYS AND ACOUSTIC WAVEFIELD IMAGING
DAMAGE DETECTION IN PLATE STRUCTURES USING SPARSE ULTRASONIC TRANSDUCER ARRAYS AND ACOUSTIC WAVEFIELD IMAGING T. E. Michaels 1,,J.E.Michaels 1,B.Mi 1 and M. Ruzzene 1 School of Electrical and Computer
More informationACOUSTIC EMISSION MEASUREMENTS ON SHELL STRUCTURES WITH DIRECTLY ATTACHED PIEZO-CERAMIC
ACOUSTIC EMISSION MEASUREMENTS ON SHELL STRUCTURES WITH DIRECTLY ATTACHED PIEZO-CERAMIC Abstract FRANZ RAUSCHER and MULU BAYRAY Institute of Pressure Vessels and Plant Technology Vienna University of Technology,
More informationTitle: Reference-free Structural Health Monitoring for Detecting Delamination in Composite Plates
Title: Reference-free Structural Health Monitoring for Detecting Delamination in Composite Plates Authors (names are for example only): Chul Min Yeum Hoon Sohn Jeong Beom Ihn Hyung Jin Lim ABSTRACT This
More informationSensitivity analysis of guided wave characters for transducer array optimisation on pipeline inspections
Sensitivity analysis of guided wave characters for transducer array optimisation on pipeline inspections Xudong Niu 1), Hugo R. Marques 2) and *Hua-Peng Chen 3) 1),3) Department of Engineering Science,
More informationGuided Wave Travel Time Tomography for Bends
18 th World Conference on Non destructive Testing, 16-20 April 2012, Durban, South Africa Guided Wave Travel Time Tomography for Bends Arno VOLKER 1 and Tim van ZON 1 1 TNO, Stieltjes weg 1, 2600 AD, Delft,
More informationvibro-acoustic modulation
17th World Conference on Nondestructive Testing, 25-28 Oct 28, Shanghai, ChinaContact defect detection in plates using guided wave and vibro-acoustic modulation Jingpin JIAO 1, Bruce W. DRINKWATER 2, Simon
More informationISO INTERNATIONAL STANDARD. Non-destructive testing Acoustic emission inspection Secondary calibration of acoustic emission sensors
INTERNATIONAL STANDARD ISO 12714 First edition 1999-07-15 Non-destructive testing Acoustic emission inspection Secondary calibration of acoustic emission sensors Essais non destructifs Contrôle par émission
More informationACOUSTO-ULTRASONIC EVALUATION OF HYBRID COMPOSITES USING
ACOUSTO-ULTRASONIC EVALUATION OF HYBRID COMPOSITES USING OBLIQUE INCIDENCE WAVES INTRODUCTION Yuyin Ji, Sotirios J. Vahaviolos, Ronnie K. Miller, Physical Acoustics Corporation P.O. Box 3135 Princeton,
More informationFinite element simulation of photoacoustic fiber optic sensors for surface rust detection on a steel rod
Finite element simulation of photoacoustic fiber optic sensors for surface rust detection on a steel rod Qixiang Tang a, Jones Owusu Twumasi a, Jie Hu a, Xingwei Wang b and Tzuyang Yu a a Department of
More informationAPPLICATION OF ULTRASONIC GUIDED WAVES FOR INVESTIGATION OF COMPOSITE CONSTRUCTIONAL COMPONENTS OF TIDAL POWER PLANTS
The 12 th International Conference of the Slovenian Society for Non-Destructive Testing»Application of Contemporary Non-Destructive Testing in Engineering«September 4-6, 2013, Portorož, Slovenia More info
More informationLong Range Ultrasonic Testing - Case Studies
More info about this article: http://www.ndt.net/?id=21145 Prawin Kumar Sharan 1, Sheethal S 1, Sri Krishna Chaitanya 1, Hari Kishore Maddi 1 1 Sievert India Pvt. Ltd. (A Bureau Veritas Company), 16 &
More informationRecommendation of RILEM TC 212-ACD: acoustic emission and related NDE techniques for crack detection and damage evaluation in concrete*
Materials and Structures (2010) 43:1177 1181 DOI 10.1617/s11527-010-9638-0 RILEM TECHNICAL COMMITTEE Recommendation of RILEM TC 212-ACD: acoustic emission and related NDE techniques for crack detection
More informationINVESTIGATION OF IMPACT DAMAGE OF CARBON FIBER- RAINFORCED PLASTIC (CFRP) BY EDDY CURRENT NON- DESTRUCTIVE TESTING
International Workshop SMART MATERIALS, STRUCTURES & NDT in AEROSPACE Conference NDT in Canada 2011 2-4 November 2011, Montreal, Quebec, Canada INVESTIGATION OF IMPACT DAMAGE OF CARBON FIBER- RAINFORCED
More informationA STUDY ON NON-CONTACT ULTRASONIC TECHNIQUE FOR ON-LINE INSPECTION OF CFRP
12 th A-PCNDT 6 Asia-Pacific Conference on NDT, 5 th 1 th Nov 6, Auckland, New Zealand A STUDY ON NON-CONTACT ULTRASONIC TECHNIQUE FOR ON-LINE INSPECTION OF CFRP Seung-Joon Lee 1, Won-Su Park 1, Joon-Hyun
More informationCIRCULAR LAMB AND LINEAR SHEAR HORIZONTAL GUIDED WAVE ARRAYS FOR STRUCTURAL HEALTH MONITORING
CIRCULAR LAMB AND LINEAR SHEAR HORIZONTAL GUIDED WAVE ARRAYS FOR STRUCTURAL HEALTH MONITORING Thomas R. Hay, Jason Van Velsor, Joseph L. Rose The Pennsylvania State University Engineering Science and Mechanics
More informationElectronic Noise Effects on Fundamental Lamb-Mode Acoustic Emission Signal Arrival Times Determined Using Wavelet Transform Results
DGZfP-Proceedings BB 9-CD Lecture 62 EWGAE 24 Electronic Noise Effects on Fundamental Lamb-Mode Acoustic Emission Signal Arrival Times Determined Using Wavelet Transform Results Marvin A. Hamstad University
More informationDevelopment of the air-coupled ultrasonic vertical reflection method
15 th Asia Pacific Conference for Non-Destructive Testing (APCNDT217), Singapore. Development of the air-coupled ultrasonic vertical reflection method M. Endo, M. Ishikawa 1, H. Nishino 1 and S.Sugimoto
More informationULTRASONIC DEFECT DETECTION IN BILLET USING TIME- OF-FLIGHT OF BOTTOM ECHO
ULTRASONIC DEFECT DETECTION IN BILLET USING TIME- OF-FLIGHT OF BOTTOM ECHO Ryusuke Miyamoto Graduate School of Systems and Information Engineering, University of Tsukuba, Tsukuba, Ibaraki 305-8573 Japan
More informationASSESSMENT OF WALL-THINNING IN CARBON STEEL PIPE BY USING LASER-GENERATED GUIDED WAVE
ASSESSMENT OF WALL-THINNING IN CARBON STEEL PIPE BY USING LASER-GENERATED GUIDED WAVE DOYOUN KIM, YOUNHO CHO * and JOONHYUN LEE Graduate School of Mechanical Engineering, Pusan National University Jangjeon-dong,
More informationSOME OBSERVATIONS ON RAYLEIGH WAVES AND ACOUSTIC EMISSION IN THICK STEEL PLATES #
SOME OBSERVATIONS ON RAYLEIGH WAVES AND ACOUSTIC EMISSION IN THICK STEEL PLATES # M. A. HAMSTAD National Institute of Standards and Technology, Materials Reliability Division (853), 325 Broadway, Boulder,
More informationHigh contrast air-coupled acoustic imaging with zero group velocity Lamb modes
Aerospace Engineering Conference Papers, Presentations and Posters Aerospace Engineering 7-3 High contrast air-coupled acoustic imaging with zero group velocity Lamb modes Stephen D. Holland Iowa State
More informationQuasi-Rayleigh Waves in Butt-Welded Thick Steel Plate
Quasi-Rayleigh Waves in Butt-Welded Thick Steel Plate Tuncay Kamas a) Victor Giurgiutiu b), Bin Lin c) a) Mechanical Engineering University of South Carolina 3 Main Str. 2928 Columbia SC b) Mechanical
More informationANALYSIS OF ACOUSTIC EMISSION FROM IMPACT AND FRACTURE OF CFRP LAMINATES
ANALYSIS OF ACOUSTIC EMISSION FROM IMPACT AND FRACTURE OF CFRP LAMINATES KANJI ONO, YOSHIHIRO MIZUTANI 1 and MIKIO TAKEMOTO 2 Department of Materials Science and Engineering, UCLA, Los Angeles, CA 90095-1595,
More informationHybrid Passive/Active Impact Detection & Localization for Aerospace Structures Seth S. Kessler and Eric B. Flynn. Metis Design Corporation
Hybrid Passive/Active Impact Detection & Localization for Aerospace Structures Seth S. Kessler and Eric B. Flynn Metis Design Corporation IWSHM-2013 ABSTRACT This paper presents finding from a recent set
More informationredefining the limits of ultrasound
redefining the limits of ultrasound Non-Contact Ultrasonic Inspection for Continuous Feedback in Manufacturing JEC Europe Paris March 12, 2013 We will explore non-contact ultrasound (NCU), the advantages
More informationID-1223 Determination of delamination onset in composite laminates by application of acoustic emission INTRODUCTION
ID-1223 Determination of delamination onset in composite laminates by application of acoustic emission Karol Kaczmarek ABB Corporate Research, Starowislna 13a, 31-038 Cracow, Poland SUMMARY: This paper
More informationAcoustic Emission Signals versus Propagation Direction for Hybrid Composite Layup with Large Stiffness Differences versus Direction
31 st Conference of the European Working Group on Acoustic Emission (EWGAE) We.1.A.1 More Info at Open Access Database www.ndt.net/?id=17568 Acoustic Emission Signals versus Propagation Direction for Hybrid
More informationAcoustic Emission For Damage Monitoring of Glass /Polyester Composites under Buckling Loading
Research Article International Journal of Current Engineering and Technology ISSN 2277-4106 2012 INPRESSCO. All Rights Reserved. Available at http://inpressco.com/category/ijcet Acoustic Emission For Damage
More informationREFLECTION AND TRANSMISSION OF LAMB WAVES AT DISCONTINUITY IN PLATE Z. Liu NDT Systems & Services AG, Stutensee, Germany
REFLECTION AND TRANSMISSION OF LAMB WAVES AT DISCONTINUITY IN PLATE Z. Liu NDT Systems & Services AG, Stutensee, Germany Abstract: Lamb waves can be used for testing thin plate and pipe because they provide
More informationSpectral Distance Amplitude Control for Ultrasonic Inspection of Composite Components
ECNDT 26 - Mo.2.6.4 Spectral Distance Amplitude Control for Ultrasonic Inspection of Composite Components Uwe PFEIFFER, Wolfgang HILLGER, DLR German Aerospace Center, Braunschweig, Germany Abstract. Ultrasonic
More informationAcoustic Emission Signal Associated to Fiber Break during a Single Fiber Fragmentation Test: Modeling and Experiment
Proceedings Acoustic Emission Signal Associated to Fiber Break during a Single Fiber Fragmentation Test: Modeling and Experiment Zeina Hamam 1, *, Nathalie Godin 1, Claudio Fusco 1 and Thomas Monnier 2
More informationDEVELOPMENT OF MEASUREMENT SYSTEM USING OPTICAL FIBER AE SENSORS FOR ACTUAL PIPING
DEVELOPMENT OF MEASUREMENT SYSTEM USING OPTICAL FIBER AE SENSORS FOR ACTUAL PIPING SATOSHI NISHINOIRI, PORNTHEP CHIVAVIBUL, HIROYUKI FUKUTOMI and TAKASHI OGATA Materials Science Research Laboratory, Central
More informationMathematical Model and Numerical Analysis of AE Wave Generated by Partial Discharges
Vol. 120 (2011) ACTA PHYSICA POLONICA A No. 4 Optical and Acoustical Methods in Science and Technology Mathematical Model and Numerical Analysis of AE Wave Generated by Partial Discharges D. Wotzka, T.
More informationLamb Wave Dispersion Compensation in Piezoelectric Wafer Active Sensor Phased-Array Applications
Lamb Wave Dispersion Compensation in Piezoelectric Wafer Active Sensor Phased-Array Applications Buli Xu, Lingyu Yu, Victor Giurgiutiu Mechanical Engineering Department, University of South Carolina Columbia,
More informationULTRASONIC GUIDED WAVE FOCUSING BEYOND WELDS IN A PIPELINE
ULTRASONI GUIDED WAVE FOUSING BEYOND WELDS IN A PIPELINE Li Zhang, Wei Luo, Joseph L. Rose Department of Engineering Science & Mechanics, The Pennsylvania State University, University Park, PA 1682 ABSTRAT.
More informationA NEW APPROACH FOR THE ANALYSIS OF IMPACT-ECHO DATA
A NEW APPROACH FOR THE ANALYSIS OF IMPACT-ECHO DATA John S. Popovics and Joseph L. Rose Department of Engineering Science and Mechanics The Pennsylvania State University University Park, PA 16802 INTRODUCTION
More informationNONDESTRUCTIVE EVALUATION OF CLOSED CRACKS USING AN ULTRASONIC TRANSIT TIMING METHOD J. Takatsubo 1, H. Tsuda 1, B. Wang 1
NONDESTRUCTIVE EVALUATION OF CLOSED CRACKS USING AN ULTRASONIC TRANSIT TIMING METHOD J. Takatsubo 1, H. Tsuda 1, B. Wang 1 1 National Institute of Advanced Industrial Science and Technology, Tsukuba, Japan
More informationAging Wire Insulation Assessment by Phase Spectrum Examination of Ultrasonic Guided Waves 1
Aging Wire Insulation Assessment by Phase Spectrum Examination of Ultrasonic Guided Waves 1 Robert F. Anastasi 1 and Eric I. Madaras 2 1 U.S. Army Research Laboratory, Vehicle Technology Directorate, AMSRL-VT-S,
More informationAbstract. 1 Introduction. 1.2 Concept. 1.1 Problematic. 1.3 Modelling
Piezo-composite transducer for mode and direction selectivity of Lamb waves Eng. Thomas Porchez, Cedrat Technologies, Meylan, France Dr. Nabil Bencheikh, Cedrat Technologies, Meylan, France Dr. Ronan Le
More informationMulti-Mode and Multi-Frequency Differential Lamb Wave Imaging with in situ Sparse Transducer Arrays
ECNDT 26 - Tu.1.3.3 Multi-Mode and Multi-Frequency Differential Lamb Wave Imaging with in situ Sparse Transducer Arrays Jennifer E. MICHAELS and Thomas E. MICHAELS, School of Electrical and Computer Engineering,
More informationA Wire-Guided Transducer for Acoustic Emission Sensing
A Wire-Guided Transducer for Acoustic Emission Sensing Ian T. Neill a, I. J. Oppenheim a*, D. W. Greve b a Dept. of Civil and Environmental Engineering, Carnegie Mellon University, Pittsburgh, PA 15213
More informationPRACTICAL ASPECTS OF ACOUSTIC EMISSION SOURCE LOCATION BY A WAVELET TRANSFORM
PRACTICAL ASPECTS OF ACOUSTIC EMISSION SOURCE LOCATION BY A WAVELET TRANSFORM Abstract M. A. HAMSTAD 1,2, K. S. DOWNS 3 and A. O GALLAGHER 1 1 National Institute of Standards and Technology, Materials
More informationAir- coupled ultrasonic testing of CFRP rods by means of guided waves
Available online at www.sciencedirect.com Physics Physics Procedia 3 (2010) 00 (2009) 185 192 000 000 www.elsevier.com/locate/procedia International Congress on Ultrasonics, Universidad de Santiago de
More informationEffect of coupling conditions on ultrasonic echo parameters
J. Pure Appl. Ultrason. 27 (2005) pp. 70-79 Effect of coupling conditions on ultrasonic echo parameters ASHOK KUMAR, NIDHI GUPTA, REETA GUPTA and YUDHISTHER KUMAR Ultrasonic Standards, National Physical
More informationAcoustic Emission Source Location Based on Signal Features. Blahacek, M., Chlada, M. and Prevorovsky, Z.
Advanced Materials Research Vols. 13-14 (6) pp 77-82 online at http://www.scientific.net (6) Trans Tech Publications, Switzerland Online available since 6/Feb/15 Acoustic Emission Source Location Based
More informationA Numerical study on proper mode and frequency selection for riveted lap joints inspection using Lamb waves.
More Info at Open Access Database www.ndt.net/?id=18676 A Numerical study on proper mode and frequency selection for riveted lap joints inspection using Lamb waves. Mohammad. (. SOORGEE Nondestructive
More informationRODS AND TUBES AS AE WAVEGUIDES
RODS AND TUBES AS AE WAVEGUIDES KANJI ONO 1 and HIDEO CHO 2 1 University of California, Los Angeles, California, USA 2 Aoyama Gakuin University, Sagamihara, Kanagawa, Japan. Abstract We have examined the
More informationUltrasonic Guided Wave Testing of Cylindrical Bars
18th World Conference on Nondestructive Testing, 16-2 April 212, Durban, South Africa Ultrasonic Guided Wave Testing of Cylindrical Bars Masanari Shoji, Takashi Sawada NTT Energy and Environment Systems
More informationINSPECTION OF THERMAL BARRIERS OF PRIMARY PUMPS WITH PHASED ARRAY PROBE AND PIEZOCOMPOSITE TECHNOLOGY
INSPECTION OF THERMAL BARRIERS OF PRIMARY PUMPS WITH PHASED ARRAY PROBE AND PIEZOCOMPOSITE TECHNOLOGY J. Poguet Imasonic S.A. France E. Abittan EDF-GDL France Abstract In order to meet the requirements
More information1818. Evaluation of arbitrary waveform acoustic signal generation techniques in dispersive waveguides
1818. Evaluation of arbitrary waveform acoustic signal generation techniques in dispersive waveguides V. Augutis 1, D. Gailius 2, E. Vastakas 3, P. Kuzas 4 Kaunas University of Technology, Institute of
More informationAUTOMATED METHOD FOR STATISTIC PROCESSING OF AE TESTING DATA
AUTOMATED METHOD FOR STATISTIC PROCESSING OF AE TESTING DATA V. A. BARAT and A. L. ALYAKRITSKIY Research Dept, Interunis Ltd., bld. 24, corp 3-4, Myasnitskaya str., Moscow, 101000, Russia Keywords: signal
More informationDamage Detection in Stiffened Composite Panels Using Lamb Wave
6th European Workshop on Structural Health Monitoring - We.2.A.4 More info about this article: http://www.ndt.net/?id=14121 Damage Detection in Stiffened Composite Panels Using Lamb Wave B. JANARTHAN,
More informationCOMPOSITES FROM PIEZOELECTRIC FIBERS AS SENSORS AND EMITTERS FOR ACOUSTIC APPLICATIONS*
COMPOSITES FROM PIEZOELECTRIC FIBERS AS SENSORS AND EMITTERS FOR ACOUSTIC APPLICATIONS* Abstract ANDREAS J. BRUNNER, MICHEL BARBEZAT, PETER FLÜELER and CHRISTIAN HUBER Polymers/Composites Laboratory, EMPA,
More informationUltrasonic Time-of-Flight Shift Measurements in Carbon Composite Laminates Containing Matrix Microcracks
Ultrasonic Time-of-Flight Shift Measurements in Carbon Composite Laminates Containing Matrix Microcracks Ajith Subramanian a, Vinay Dayal b, and Daniel J. Barnard a a CNDE, Iowa State University, Ames,
More informationINTERNAL CONCRETE INSPECTION AND EVALUATION METHODS FOR STEEL PLATE-BONDED SLABS BY USING ELASTIC WAVES VIA ANCHOR BOLTS
More info about this article: h Czech Society for Nondestructive Testing 32 nd European Conference on Acoustic Emission Testing Prague, Czech Republic, September 7-9, 216 INTERNAL CONCRETE INSPECTION AND
More informationOPTIMAL EXCITATION FREQUENCY FOR DELAMINATION IDENTIFICATION OF LAMINATED BEAMS USING A 0 LAMB MODE
OPTIMAL EXCITATION FREQUENCY FOR DELAMINATION IDENTIFICATION OF LAMINATED BEAMS USING A 0 LAMB MODE N. Hu 1 *, H. Fukunaga 2, Y. Liu 3 and Y. Koshin 2 1 Department of Mechanical Engineering, Chiba University,
More informationA SHEAR WAVE TRANSDUCER ARRAY FOR REAL-TIME IMAGING. R.L. Baer and G.S. Kino. Edward L. Ginzton Laboratory Stanford University Stanford, CA 94305
A SHEAR WAVE TRANSDUCER ARRAY FOR REAL-TIME IMAGING R.L. Baer and G.S. Kino Edward L. Ginzton Laboratory Stanford University Stanford, CA 94305 INTRODUCTION In this paper we describe a contacting shear
More informationRECENT ADVANCEMENTS IN THE APPLICATION OF EMATS TO NDE
RECENT ADVANCEMENTS IN THE APPLICATION OF EMATS TO NDE D. MacLauchlan, S. Clark, B. Cox, T. Doyle, B. Grimmett, J. Hancock, K. Hour, C. Rutherford BWXT Services, Non Destructive Evaluation and Inspection
More informationULTRASONIC SIGNAL CHARACTERIZATIONS OF FLAT-BOTTOM HOLES IN
ULTRASONIC SIGNAL CHARACTERIZATIONS OF FLAT-BOTTOM HOLES IN TITANIUM ALLOYS: EXPERIMENT AND THEORY INTRODUCTION Chien-Ping Chiou 1, Frank J. Margetan 1 and R. Bruce Thompson2 1 FAA Center for Aviation
More informationAssessment of lamination defect near the inner surface based on quasi-symmetric circumferential Lamb waves
5 th Asia Pacific Conference for Non-Destructive Testing (APCNDT27), Singapore. Assessment of lamination defect near the inner surface based on quasi-symmetric circumferential Lamb waves Ziming Li, Cunfu
More informationAcquisition and Analysis of Continuous Acoustic Emission Waveform for Classification of Damage Sources in Ceramic Fiber Mat
Materials Transactions, Vol. 48, No. 6 (27) pp. 1221 to 1226 Special Issue on Advances in Non-Destructive Inspection and Materials Evaluation #27 The Japanese Society for Non-Destructive Inspection Acquisition
More informationInvestigation of Woven Fiber Reinforced Laminated Composites Using a Through Transmission Ultrasonic Technique
Photos placed in horizontal position with even amount of white space between photos and header Photos placed in horizontal position with even amount of white space between photos and header Investigation
More informationUltrasonic Testing using a unipolar pulse
Ultrasonic Testing using a unipolar pulse by Y. Udagawa* and T. Shiraiwa** *Imaging Supersonic Laboratories Co.,Ltd. 12-7 Tezukayamanakamachi Nara Japan 63163 1. Abstract Krautkramer Japan Co.,Ltd. 9-29
More informationAbsolute Calibration of Acoustic Emission Transducers as per CEN ISO/TR in Disuse of Mechanical Sound Sources or Reference Transducers
30th European Conference on Acoustic Emission Testing & 7th International Conference on Acoustic Emission University of Granada, 12-15 September 2012 Absolute Calibration of Acoustic Emission Transducers
More informationIn-Situ Damage Detection of Composites Structures using Lamb Wave Methods
In-Situ Damage Detection of Composites Structures using Lamb Wave Methods Seth S. Kessler S. Mark Spearing Mauro J. Atalla Technology Laboratory for Advanced Composites Department of Aeronautics and Astronautics
More informationMEASUREMENT OF SURFACE DISPLACEMENT EXCITED BY EMAT TRANSDUCER
XIX IMEKO World Congress Fundamental and Applied Metrology September 6 11, 29, Lisbon, Portugal MEASUREMENT OF SURFACE DISPLACEMENT EXCITED BY EMAT TRANSDUCER Petr Fidler 1, Petr Beneš 2 1 Brno University
More informationMaximizing the Fatigue Crack Response in Surface Eddy Current Inspections of Aircraft Structures
Maximizing the Fatigue Crack Response in Surface Eddy Current Inspections of Aircraft Structures Catalin Mandache *1, Theodoros Theodoulidis 2 1 Structures, Materials and Manufacturing Laboratory, National
More informationIMAGING OF DEFECTS IN CONCRETE COMPONENTS WITH NON-CONTACT ULTRASONIC TESTING W. Hillger, DLR and Ing. Büro Dr. Hillger, Braunschweig, Germany
IMAGING OF DEFECTS IN CONCRETE COMPONENTS WITH NON-CONTACT ULTRASONIC TESTING W. Hillger, DLR and Ing. Büro Dr. Hillger, Braunschweig, Germany Abstract: The building industries require NDT- methods for
More informationExperimental Application of Optimized Lamb Wave Actuating/Sensing Patches for Health Monitoring of Composite Structures
Experimental Application of Optimized Lamb Wave Actuating/Sensing Patches for Health Monitoring of Composite Structures Seth S. Kessler and Christopher E. Johnson Metis Design Corporation Christopher T.
More informationCONTACT LASER ULTRASONIC EVALUATION OF CONSTRUCTION MATERIALS
CONTACT LASER ULTRASONIC EVALUATION OF CONSTRUCTION MATERIALS Alexander A.KARABUTOV 1, Elena V.SAVATEEVA 2, Alexei N. ZHARINOV 1, Alexander A.KARABUTOV 1 Jr. 1 International Laser Center of M.V.Lomonosov
More informationNUMERICAL MODELING OF AIR-COUPLED ULTRASOUND WITH EFIT. D. E. Chimenti Center of Nondestructive Evaluation Iowa State University Ames, Iowa, USA
NUMERICAL MODELING OF AIR-COUPLED ULTRASOUND WITH EFIT M. Rudolph, P. Fellinger and K. J. Langenberg Dept. Electrical Engineering University of Kassel 34109 Kassel, Germany D. E. Chimenti Center of Nondestructive
More information1831. Fractional derivative method to reduce noise and improve SNR for lamb wave signals
8. Fractional derivative method to reduce noise and improve SNR for lamb wave signals Xiao Chen, Yang Gao, Chenlong Wang Jiangsu Key Laboratory of Meteorological observation and Information Processing,
More informationSummary. D Receiver. Borehole. Borehole. Borehole. tool. tool. tool
n off center quadrupole acoustic wireline : numerical modeling and field data analysis Zhou-tuo Wei*, OSL-UP llied coustic Lab., hina University of Petroleum (UP); Hua Wang, Earth Resources Lab., Massachusetts
More informationGeneration Laser Scanning Method for Visualizing Ultrasonic Waves Propagating on a 3-D Object
1st International Symposium on Laser Ultrasonics: Science, Technology and Applications July 16-18 2008, Montreal, Canada Generation Laser Scanning Method for Visualizing Ultrasonic Waves Propagating on
More informationDesign of mode selective actuators for Lamb wave excitation in composite plates
CEAS Aeronaut J DOI 10.1007/s13272-012-0059-3 ORIGINAL PAPER Design of mode selective actuators for Lamb wave excitation in composite plates Daniel Schmidt Michael Sinapius Peter Wierach Received: 12 April
More information